1 / 18

Measuring Spin-Orbit Alignment of Transiting Exoplanets with Subaru/HDS

Measuring Spin-Orbit Alignment of Transiting Exoplanets with Subaru/HDS. Norio Narita National Astronomical Observatory of Japan. Outline. Backgrounds Planetary orbital distribution Planetary migration models The Rossiter effect Subaru observations and results

maia
Download Presentation

Measuring Spin-Orbit Alignment of Transiting Exoplanets with Subaru/HDS

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Measuring Spin-Orbit Alignmentof Transiting Exoplanetswith Subaru/HDS Norio Narita National Astronomical Observatory of Japan

  2. Outline • Backgrounds • Planetary orbital distribution • Planetary migration models • The Rossiter effect • Subaru observations and results • Discussions and summary

  3. Semi-Major Axis Distribution of Exoplanets Snow line Jupiter Need planetary migration mechanisms!

  4. Standard Migration Models Type I and II migration mechanisms • consider gravitational interaction between • proto-planetary disk • planets • Type I: less than 10 Earth mass proto-planet • Type II: more massive case • well explain the semi-major axis distribution • e.g., a series of Ida & Lin papers • predict small eccentricities for migrated planets

  5. Eccentricity Distribution Eccentric Planets Jupiter Cannot be explained by Type I & II migration model.

  6. Migration Models for Eccentric Planets • consider gravitational interaction between • planet-planet (planet-planet scattering models) • planet-binary companion (the Kozai migration) • Cf. Kozai-san = the first NAOJ director • may be able to explain eccentricity distribution • e.g., Nagasawa+ 2008, Chatterjee+ 2008 • predict a variety of eccentricities and misalignments between stellar spin and planetary orbital axes • How can we confirm these models by observations?

  7. The Rossiter Effect for Transiting Planets When a transiting planet hides stellar rotation, star planet planet hide approaching side → appear to be receding hide receding side → appear to be approaching radial velocity of the host star would show an anomaly.

  8. What can we learn from the effect? The shape of the Rossiter effect depends on the trajectory of the transiting planet. misaligned well aligned Radial velocity = Keplerian motion + Rossiter effect Gaudi & Winn (2007)

  9. Spin-Orbit Alignment λ： sky-projected angle between the stellar spin axis and the planetary orbital axis (e.g., Ohta et al. 2005, Gimentz 2006, Gaudi & Winn 2007)

  10. Past Subaru Observations • Proposals and target list • S06A-029: TrES-1 • S07A-007: TrES-4 • S07B-091: TrES-3, WASP-1, WASP-2, HAT-P-1 • S08A-021: XO-2, HAT-P-7 • S08B-086: XO-3 • S08B-087: HD17156 • Blue: Planets in Binary System / Green: Eccentric Planets

  11. TrES-1: Slow Rotation and Faint Target Our first observation with Subaru/HDS – difficult target NN et al. (2007) Thanks to Subaru, clear detection of the Rossiter effect. We confirmed a prograde orbit and alignment of the planet.

  12. TrES-3: Slower and Fainter Target More difficult target NN et al. in prep. Very weak detection of the Rossiter effect. This planet also orbits in a prograde and aligned way.

  13. TrES-4: Fast Rotating Binary Target The Rossiter effect is greater than the Keplerian motion! NN et al. in prep. Well aligned in spite of its binarity.

  14. HD17156: Eccentric Target Eccentric planet with the orbital period of 21.2 days. NN et al. (2009) Aligned in spite of its eccentricity.

  15. XO-3: Another Eccentric Target Hebrard et al. (2008) λ = 70 ± 15 deg Large misalignmentswere reported, but not yet confirmed. (2σ discrepancy) Winn et al. (2009) λ = 37.3 ± 3.7 deg Unfortunately S08B Subaru observation failed due to bad weather.

  16. List of Previous Studies • HD209458 Queloz et al. 2000, Winn et al. 2005 • HD189733 Winn et al. 2006 • TrES-1 NN+ 2007 • HAT-P-2 Winn et al. 2007, Loeillet et al. 2008 • HD149026 Wolf et al. 2007 • HD17156 NN+ 2008,2009, Cochran+ 2008, Barbieri+ 2009 • TrES-2 Winn et al. 2008 • CoRoT-Exo-2 Bouchy et al. 2008 • HAT-P-1 Johnson et al. 2008 • XO-3 Hebrard et al. 2008, Winn et al. 2009 • WASP-14 Joshi et al. 2008 • (TrES-3, 4, WASP-1, 2, HAT-P-7, XO-2 NN+ in prep.)

  17. Statistical Study • Fabrycky and Winn (2009) considered two models, • A perfectly aligned (with large dispersion) distribution • Corresponding to Type II migration model • Aligned distribution + partly isotropic distribution • Corresponding to a combination of migration models • Winn et al. (2009) reported • The second model is preferred with a confidence of 96.6% • But it is not robust because XO-3 is the only one sample • More samples needed

  18. Summary and Future Prospects • So far almost all planets show no large misalignment • consistent with standard Type II migration models • HD17156b (eccentric planet) also show no misalignment • Only 1 exception is XO-3b • λ= 70 ± 15 deg (Hebrard et al. 2008) • λ= 37.3 ± 3.7 deg (Winn et al. 2009) • formed through planet-planet scattering? • Statistical study is just beginning • More samples (especially eccentric planets) needed • The Rossiter effect is useful to study planet migration!

More Related